Chern--Simons Perturbation Theory II

dc.creatorAxelrod, Scott
dc.creatorSinger, I. M.
dc.date1993-04-21
dc.date.accessioned2026-07-07T09:14:02Z
dc.date.available2026-07-07T09:14:02Z
dc.descriptionIn a previous paper [\AS], we used superspace techniques to prove that perturbation theory (around a classical solution with no zero modes) for Chern--Simons quantum field theory on a general $3$-manifold $M$ is finite. We conjectured (and proved for the case of $2$-loops) that, after adding counterterms of the expected form, the terms in the perturbation theory define topological invariants. In this paper we prove this conjecture. Our proof uses a geometric compactification of the region on which the Feynman integrand of Feynman diagrams is smooth as well as an extension of the basic propagator of the theory.
dc.description40 pages
dc.identifierhttps://arxiv.org/abs/hep-th/9304087
dc.identifierhttp://arxiv.org/abs/hep-th/9304087
dc.identifierJ.Diff.Geom. 39 (1994) 173-213
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/152533
dc.subjectHigh Energy Physics - Theory
dc.subjectDifferential Geometry
dc.subjectQuantum Algebra
dc.titleChern--Simons Perturbation Theory II
dc.typetext

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